ENTRY C2088 20140123 C139C208800000001 SUBENT C2088001 20140123 C139C208800100001 BIB 8 26 C208800100002 TITLE Reactions of a 10Be beam on proton and deuteron targetsC208800100003 AUTHOR (K.T.Schmitt,K.L.Jones,S.Ahn,D.W.Bardayan,A.Bey, C208800100004 J.C.Blackmon,S.M.Brown,K.Y.Chae,K.A.Chipps, C208800100005 J.A.Cizewski,K.I.Hahn,J.J.Kolata,R.L.Kozub,J.F.Liang, C208800100006 C.Matei,M.Matos,D.Matyas,B.Moazen,C.D.Nesaraja, C208800100007 F.M.Nunes,P.D.O'Malley,S.D.Pain,W.A.Peters,S.T.Pittman,C208800100008 A.Roberts,D.Shapira,J.F.Shriner Jr,M.S.Smith, C208800100009 I.Spassova,D.W.Stracener,N.J.Upadhyay,A.N.Villano, C208800100010 G.L.Wilson) C208800100011 INSTITUTE (1USATEN,1USAMSU,1USAORL,1USANOT,1USALSU,2UK SUR, C208800100012 1USARUT,1USATTU,1USAOAU,1USADNS,1USAWMU,1USACSM) C208800100013 (3KORKOR) Sungkyunkwan University, Suwon C208800100014 (3KORKOR) Ewha Womans University,Seoul C208800100015 REFERENCE (J,PR/C,88,064612,2013) C208800100016 FACILITY (VDGT,1USAORL) Experiment performed using 25-MV C208800100017 tandem accelerator at HRIBF facility at Oak Ridge C208800100018 National Laboratory C208800100019 METHOD Experiment performed in inverse kinematics at 10Be beamC208800100020 energies of 60, 75, 90, and 107 MeV, equivalent to C208800100021 12, 15, 18, and 21.4 MeV deuteron energies and C208800100022 6, 7.5, 9, and 10.7 MeV proton energies. Only C208800100023 equivalent energies are given in all subentries. C208800100024 ERR-ANALYS (ERR-1) Systematic uncertainty in solid angle coverage C208800100025 (ERR-2) Syst. uncertainty in beam counting measurement C208800100026 (ERR-3) Syst. uncertainty in target thickness C208800100027 HISTORY (20140123C) Compiled by S.H. C208800100028 ENDBIB 26 0 C208800100029 COMMON 3 3 C208800100030 ERR-1 ERR-2 ERR-3 C208800100031 PER-CENT PER-CENT PER-CENT C208800100032 3.0 5.0 5.0 C208800100033 ENDCOMMON 3 0 C208800100034 ENDSUBENT 33 0 C208800199999 SUBENT C2088002 20140123 C139C208800200001 BIB 5 23 C208800200002 REACTION (4-BE-10(P,EL)4-BE-10,,DA,,RTH) C208800200003 STATUS (TABLE) Data presented in fig. 2 of the reference takenC208800200004 from tabulated data given in Supplemental Material at C208800200005 http: C208800200006 //link.aps.org/supplemental/10.1103/PhysRevC.88.064612 C208800200007 SAMPLE The CH2 target was prepared from commercially C208800200008 available polyethylene sheets, stretched to achieve C208800200009 an areal density of 226 mu-g/cm2. The thickness of C208800200010 each target was measured using the energy loss of C208800200011 5.805-MeV alpha particles from the decay of 244Cm. C208800200012 DETECTOR (MCPLT) A new dual microchannel plate (DMCP) detector C208800200013 was employed for heavy recoil detection. The DMCP C208800200014 utilizes two conventional MCP detectors viewing C208800200015 opposing sides of a single carbon or metallized foil. C208800200016 (SI) SuperORRUBA detectors, which are segmented for C208800200017 1.2-mm position sensitivity, were used at angles C208800200018 forward of 90deg for the proton scattering measurementsC208800200019 ERR-ANALYS (ERR-4) Syst. uncertainty in sieve rate C208800200020 (ERR-5) Syst. uncert. in normalization run statistics C208800200021 (ERR-6) Systematic uncertainty in normalization gating C208800200022 (ERR-T) Total uncertainty C208800200023 (ERR-S) Combined uncertainty from counting statistics C208800200024 and Gaussian fits binned angular data C208800200025 ENDBIB 23 0 C208800200026 COMMON 5 3 C208800200027 EN ERR-4 ERR-5 ERR-6 ERR-T C208800200028 MEV PER-CENT PER-CENT PER-CENT PER-CENT C208800200029 6.0 0.0 6.0 0.0 8.0 C208800200030 ENDCOMMON 3 0 C208800200031 DATA 3 24 C208800200032 ANG-CM DATA ERR-S C208800200033 ADEG NO-DIM NO-DIM C208800200034 28.9 2.1 0.20 C208800200035 30.1 2.3 0.20 C208800200036 31.3 2.4 0.10 C208800200037 32.5 2.7 0.10 C208800200038 33.6 2.8 0.10 C208800200039 34.8 2.8 0.10 C208800200040 35.9 2.9 0.10 C208800200041 37.0 3.3 0.10 C208800200042 38.2 3.3 0.10 C208800200043 39.3 3.8 0.10 C208800200044 40.6 3.8 0.10 C208800200045 42.0 4.2 0.20 C208800200046 43.1 3.8 0.20 C208800200047 44.2 4.3 0.20 C208800200048 45.3 4.3 0.20 C208800200049 46.4 4.2 0.20 C208800200050 47.4 4.6 0.20 C208800200051 48.5 4.5 0.20 C208800200052 49.5 5.2 0.20 C208800200053 50.5 4.6 0.20 C208800200054 51.8 4.5 0.20 C208800200055 53.4 4.7 0.20 C208800200056 54.7 4.6 0.20 C208800200057 56.0 4.7 0.30 C208800200058 ENDDATA 26 0 C208800200059 ENDSUBENT 58 0 C208800299999 SUBENT C2088003 20140123 C139C208800300001 BIB 5 23 C208800300002 REACTION (4-BE-10(P,EL)4-BE-10,,DA,,RTH) C208800300003 STATUS (TABLE) Data presented in fig. 2 of the reference takenC208800300004 from tabulated data given in Supplemental Material at C208800300005 http: C208800300006 //link.aps.org/supplemental/10.1103/PhysRevC.88.064612 C208800300007 SAMPLE The CH2 target was prepared from commercially C208800300008 available polyethylene sheets, stretched to achieve C208800300009 an areal density of 226 mu-g/cm2. The thickness of C208800300010 each target was measured using the energy loss of C208800300011 5.805-MeV alpha particles from the decay of 244Cm. C208800300012 DETECTOR (MCPLT) A new dual microchannel plate (DMCP) detector C208800300013 was employed for heavy recoil detection. The DMCP C208800300014 utilizes two conventional MCP detectors viewing C208800300015 opposing sides of a single carbon or metallized foil. C208800300016 (SI) SuperORRUBA detectors, which are segmented for C208800300017 1.2-mm position sensitivity, were used at angles C208800300018 forward of 90deg for the proton scattering measurementsC208800300019 ERR-ANALYS (ERR-4) Syst. uncertainty in sieve rate C208800300020 (ERR-5) Syst. uncert. in normalization run statistics C208800300021 (ERR-6) Systematic uncertainty in normalization gating C208800300022 (ERR-T) Total uncertainty C208800300023 (ERR-S) Combined uncertainty from counting statistics C208800300024 and Gaussian fits binned angular data C208800300025 ENDBIB 23 0 C208800300026 COMMON 5 3 C208800300027 EN ERR-4 ERR-5 ERR-6 ERR-T C208800300028 MEV PER-CENT PER-CENT PER-CENT PER-CENT C208800300029 7.5 7.0 5.0 0.0 12.0 C208800300030 ENDCOMMON 3 0 C208800300031 DATA 3 25 C208800300032 ANG-CM DATA ERR-S C208800300033 ADEG NO-DIM NO-DIM C208800300034 27.8 2.3 0.05 C208800300035 28.9 2.8 0.04 C208800300036 30.1 3.3 0.05 C208800300037 31.3 3.6 0.06 C208800300038 32.5 3.9 0.06 C208800300039 33.6 4.2 0.07 C208800300040 34.8 4.5 0.07 C208800300041 35.9 4.7 0.08 C208800300042 37.0 5.0 0.09 C208800300043 38.2 5.2 0.10 C208800300044 39.3 5.5 0.10 C208800300045 40.6 5.8 0.09 C208800300046 42.0 6.1 0.12 C208800300047 43.1 6.4 0.13 C208800300048 44.2 6.5 0.14 C208800300049 45.3 6.0 0.14 C208800300050 46.4 6.6 0.20 C208800300051 47.4 6.3 0.20 C208800300052 48.5 6.8 0.20 C208800300053 49.5 6.7 0.20 C208800300054 50.5 6.4 0.20 C208800300055 51.8 6.1 0.20 C208800300056 53.4 6.1 0.20 C208800300057 54.7 5.9 0.20 C208800300058 56.0 5.9 0.20 C208800300059 ENDDATA 27 0 C208800300060 ENDSUBENT 59 0 C208800399999 SUBENT C2088004 20140123 C139C208800400001 BIB 5 23 C208800400002 REACTION (4-BE-10(P,EL)4-BE-10,,DA,,RTH) C208800400003 STATUS (TABLE) Data presented in fig. 2 of the reference takenC208800400004 from tabulated data given in Supplemental Material at C208800400005 http: C208800400006 //link.aps.org/supplemental/10.1103/PhysRevC.88.064612 C208800400007 SAMPLE The CH2 target was prepared from commercially C208800400008 available polyethylene sheets, stretched to achieve C208800400009 an areal density of 226 mu-g/cm2. The thickness of C208800400010 each target was measured using the energy loss of C208800400011 5.805-MeV alpha particles from the decay of 244Cm. C208800400012 DETECTOR (MCPLT) A new dual microchannel plate (DMCP) detector C208800400013 was employed for heavy recoil detection. The DMCP C208800400014 utilizes two conventional MCP detectors viewing C208800400015 opposing sides of a single carbon or metallized foil. C208800400016 (SI) SuperORRUBA detectors, which are segmented for C208800400017 1.2-mm position sensitivity, were used at angles C208800400018 forward of 90deg for the proton scattering measurementsC208800400019 ERR-ANALYS (ERR-4) Syst. uncertainty in sieve rate C208800400020 (ERR-5) Syst. uncert. in normalization run statistics C208800400021 (ERR-6) Systematic uncertainty in normalization gating C208800400022 (ERR-T) Total uncertainty C208800400023 (ERR-S) Combined uncertainty from counting statistics C208800400024 and Gaussian fits binned angular data C208800400025 ENDBIB 23 0 C208800400026 COMMON 5 3 C208800400027 EN ERR-4 ERR-5 ERR-6 ERR-T C208800400028 MEV PER-CENT PER-CENT PER-CENT PER-CENT C208800400029 9.0 0.0 3.0 0.0 8.0 C208800400030 ENDCOMMON 3 0 C208800400031 DATA 3 25 C208800400032 ANG-CM DATA ERR-S C208800400033 ADEG NO-DIM NO-DIM C208800400034 27.8 3.5 0.09 C208800400035 28.9 4.0 0.08 C208800400036 30.1 4.4 0.09 C208800400037 31.3 4.9 0.10 C208800400038 32.5 5.1 0.11 C208800400039 33.6 5.7 0.12 C208800400040 34.8 5.8 0.13 C208800400041 35.9 6.1 0.14 C208800400042 37.0 6.4 0.20 C208800400043 38.2 7.0 0.20 C208800400044 39.3 7.1 0.20 C208800400045 40.6 7.6 0.20 C208800400046 42.0 7.7 0.20 C208800400047 43.1 7.8 0.20 C208800400048 44.2 7.6 0.20 C208800400049 45.3 8.2 0.30 C208800400050 46.4 8.3 0.30 C208800400051 47.4 8.1 0.30 C208800400052 48.5 8.5 0.30 C208800400053 49.5 8.9 0.30 C208800400054 50.5 8.3 0.30 C208800400055 51.8 8.2 0.30 C208800400056 53.4 7.7 0.30 C208800400057 54.7 7.5 0.30 C208800400058 56.0 7.3 0.40 C208800400059 ENDDATA 27 0 C208800400060 ENDSUBENT 59 0 C208800499999 SUBENT C2088005 20140123 C139C208800500001 BIB 5 23 C208800500002 REACTION (4-BE-10(P,EL)4-BE-10,,DA,,RTH) C208800500003 STATUS (TABLE) Data presented in fig. 2 of the reference takenC208800500004 from tabulated data given in Supplemental Material at C208800500005 http: C208800500006 //link.aps.org/supplemental/10.1103/PhysRevC.88.064612 C208800500007 SAMPLE The CH2 target was prepared from commercially C208800500008 available polyethylene sheets, stretched to achieve C208800500009 an areal density of 226 mu-g/cm2. The thickness of C208800500010 each target was measured using the energy loss of C208800500011 5.805-MeV alpha particles from the decay of 244Cm. C208800500012 DETECTOR (MCPLT) A new dual microchannel plate (DMCP) detector C208800500013 was employed for heavy recoil detection. The DMCP C208800500014 utilizes two conventional MCP detectors viewing C208800500015 opposing sides of a single carbon or metallized foil. C208800500016 (SI) SuperORRUBA detectors, which are segmented for C208800500017 1.2-mm position sensitivity, were used at angles C208800500018 forward of 90deg for the proton scattering measurementsC208800500019 ERR-ANALYS (ERR-4) Syst. uncertainty in sieve rate C208800500020 (ERR-5) Syst. uncert. in normalization run statistics C208800500021 (ERR-6) Systematic uncertainty in normalization gating C208800500022 (ERR-T) Total uncertainty C208800500023 (ERR-S) Combined uncertainty from counting statistics C208800500024 and Gaussian fits binned angular data C208800500025 ENDBIB 23 0 C208800500026 COMMON 5 3 C208800500027 EN ERR-4 ERR-5 ERR-6 ERR-T C208800500028 MEV PER-CENT PER-CENT PER-CENT PER-CENT C208800500029 10.7 0.0 2.0 0.0 8.0 C208800500030 ENDCOMMON 3 0 C208800500031 DATA 3 26 C208800500032 ANG-CM DATA ERR-S C208800500033 ADEG NO-DIM NO-DIM C208800500034 26.5 4.3 0.11 C208800500035 27.8 5.1 0.12 C208800500036 28.9 5.4 0.10 C208800500037 30.1 6.0 0.11 C208800500038 31.3 6.6 0.13 C208800500039 32.5 6.8 0.14 C208800500040 33.6 7.1 0.15 C208800500041 34.8 7.8 0.20 C208800500042 35.9 8.0 0.20 C208800500043 37.0 8.8 0.20 C208800500044 38.2 9.0 0.20 C208800500045 39.3 8.9 0.20 C208800500046 40.6 9.5 0.20 C208800500047 42.0 9.5 0.30 C208800500048 43.1 10.0 0.30 C208800500049 44.2 10.1 0.30 C208800500050 45.3 9.4 0.30 C208800500051 46.4 9.5 0.30 C208800500052 47.4 9.3 0.30 C208800500053 48.5 9.4 0.40 C208800500054 49.5 9.2 0.40 C208800500055 50.5 9.4 0.40 C208800500056 51.8 7.7 0.30 C208800500057 53.4 8.2 0.40 C208800500058 54.7 7.1 0.50 C208800500059 56.0 6.1 0.60 C208800500060 ENDDATA 28 0 C208800500061 ENDSUBENT 60 0 C208800599999 SUBENT C2088006 20140123 C139C208800600001 BIB 5 30 C208800600002 REACTION (4-BE-10(D,EL)4-BE-10,,DA,,RTH) C208800600003 STATUS (TABLE) Data presented in fig. 3 of the reference takenC208800600004 from tabulated data given in Supplemental Material at C208800600005 http: C208800600006 //link.aps.org/supplemental/10.1103/PhysRevC.88.064612 C208800600007 SAMPLE The CD2 targets were prepared from deuterated C208800600008 polyethylene powder with areal densities of 94, 143, C208800600009 162, and 185 mu-g/cm2. The thickness of each target C208800600010 was measured using the energy loss of 5.805-MeV alpha C208800600011 particles from the decay of 244Cm. C208800600012 DETECTOR (MCPLT) A new dual microchannel plate (DMCP) detector C208800600013 was employed for heavy recoil detection. The DMCP C208800600014 utilizes two conventional MCP detectors viewing C208800600015 opposing sides of a single carbon or metallized foil. C208800600016 (SI) For the data taken with deuterated targets, the C208800600017 angles and energies of light ion ejectiles were C208800600018 measured using the Silicon Detector Array (SIDAR) and C208800600019 the first full implementation of the Oak Ridge C208800600020 Rutgers Barrel Array (ORRUBA). ORRUBA detectors (1000 C208800600021 mu-m thick) were mounted at a radius of 87 mm from C208800600022 the beam axis at theta(lab) > 95 deg and at 76 mm at C208800600023 more forward angles. SIDAR array was mounted in C208800600024 lampshade configuration at backward angles to cover C208800600025 angles between 135deg and 165deg. C208800600026 ERR-ANALYS (ERR-4) Syst. uncertainty in sieve rate C208800600027 (ERR-5) Syst. uncert. in normalization run statistics C208800600028 (ERR-6) Systematic uncertainty in normalization gating C208800600029 (ERR-T) Total uncertainty C208800600030 (ERR-S) Combined uncertainty from counting statistics C208800600031 and Gaussian fits of binned angular data C208800600032 ENDBIB 30 0 C208800600033 COMMON 5 3 C208800600034 EN ERR-4 ERR-5 ERR-6 ERR-T C208800600035 MEV PER-CENT PER-CENT PER-CENT PER-CENT C208800600036 12.0 1.0 6.0 5.0 11.0 C208800600037 ENDCOMMON 3 0 C208800600038 DATA 3 12 C208800600039 ANG-CM DATA ERR-S C208800600040 ADEG NO-DIM NO-DIM C208800600041 33.2 5.74 0.15 C208800600042 35.7 4.44 0.19 C208800600043 38.1 2.69 0.18 C208800600044 40.4 1.40 0.15 C208800600045 43.8 0.12 0.10 C208800600046 47.0 1.23 0.13 C208800600047 50.2 2.67 0.30 C208800600048 53.4 4.17 0.25 C208800600049 56.6 4.76 0.30 C208800600050 59.8 5.09 0.21 C208800600051 63.0 5.02 0.17 C208800600052 66.2 5.45 0.31 C208800600053 ENDDATA 14 0 C208800600054 ENDSUBENT 53 0 C208800699999 SUBENT C2088007 20140123 C139C208800700001 BIB 5 30 C208800700002 REACTION (4-BE-10(D,EL)4-BE-10,,DA,,RTH) C208800700003 STATUS (TABLE) Data presented in fig. 3 of the reference takenC208800700004 from tabulated data given in Supplemental Material at C208800700005 http: C208800700006 //link.aps.org/supplemental/10.1103/PhysRevC.88.064612 C208800700007 SAMPLE The CD2 targets were prepared from deuterated C208800700008 polyethylene powder with areal densities of 94, 143, C208800700009 162, and 185 mu-g/cm2. The thickness of each target C208800700010 was measured using the energy loss of 5.805-MeV alpha C208800700011 particles from the decay of 244Cm. C208800700012 DETECTOR (MCPLT) A new dual microchannel plate (DMCP) detector C208800700013 was employed for heavy recoil detection. The DMCP C208800700014 utilizes two conventional MCP detectors viewing C208800700015 opposing sides of a single carbon or metallized foil. C208800700016 (SI) For the data taken with deuterated targets, the C208800700017 angles and energies of light ion ejectiles were C208800700018 measured using the Silicon Detector Array (SIDAR) and C208800700019 the first full implementation of the Oak Ridge C208800700020 Rutgers Barrel Array (ORRUBA). ORRUBA detectors (1000 C208800700021 mu-m thick) were mounted at a radius of 87 mm from C208800700022 the beam axis at theta(lab) > 95 deg and at 76 mm at C208800700023 more forward angles. SIDAR array was mounted in C208800700024 lampshade configuration at backward angles to cover C208800700025 angles between 135deg and 165deg. C208800700026 ERR-ANALYS (ERR-4) Syst. uncertainty in sieve rate C208800700027 (ERR-5) Syst. uncert. in normalization run statistics C208800700028 (ERR-6) Systematic uncertainty in normalization gating C208800700029 (ERR-T) Total uncertainty C208800700030 (ERR-S) Combined uncertainty from counting statistics C208800700031 and Gaussian fits of binned angular data C208800700032 ENDBIB 30 0 C208800700033 COMMON 5 3 C208800700034 EN ERR-4 ERR-5 ERR-6 ERR-T C208800700035 MEV PER-CENT PER-CENT PER-CENT PER-CENT C208800700036 15.0 1.0 6.0 5.0 10.0 C208800700037 ENDCOMMON 3 0 C208800700038 DATA 3 12 C208800700039 ANG-CM DATA ERR-S C208800700040 ADEG NO-DIM NO-DIM C208800700041 31.8 5.88 0.11 C208800700042 33.9 4.13 0.11 C208800700043 36.0 2.67 0.12 C208800700044 37.9 1.45 0.10 C208800700045 39.7 0.46 0.10 C208800700046 40.6 0.23 0.07 C208800700047 43.8 0.71 0.18 C208800700048 47.0 2.64 0.16 C208800700049 50.2 4.25 0.21 C208800700050 53.4 5.42 0.25 C208800700051 56.5 6.55 0.51 C208800700052 59.7 6.40 0.60 C208800700053 ENDDATA 14 0 C208800700054 ENDSUBENT 53 0 C208800799999 SUBENT C2088008 20140123 C139C208800800001 BIB 5 30 C208800800002 REACTION (4-BE-10(D,EL)4-BE-10,,DA,,RTH) C208800800003 STATUS (TABLE) Data presented in fig. 3 of the reference takenC208800800004 from tabulated data given in Supplemental Material at C208800800005 http: C208800800006 //link.aps.org/supplemental/10.1103/PhysRevC.88.064612 C208800800007 SAMPLE The CD2 targets were prepared from deuterated C208800800008 polyethylene powder with areal densities of 94, 143, C208800800009 162, and 185 mu-g/cm2. The thickness of each target C208800800010 was measured using the energy loss of 5.805-MeV alpha C208800800011 particles from the decay of 244Cm. C208800800012 DETECTOR (MCPLT) A new dual microchannel plate (DMCP) detector C208800800013 was employed for heavy recoil detection. The DMCP C208800800014 utilizes two conventional MCP detectors viewing C208800800015 opposing sides of a single carbon or metallized foil. C208800800016 (SI) For the data taken with deuterated targets, the C208800800017 angles and energies of light ion ejectiles were C208800800018 measured using the Silicon Detector Array (SIDAR) and C208800800019 the first full implementation of the Oak Ridge C208800800020 Rutgers Barrel Array (ORRUBA). ORRUBA detectors (1000 C208800800021 mu-m thick) were mounted at a radius of 87 mm from C208800800022 the beam axis at theta(lab) > 95 deg and at 76 mm at C208800800023 more forward angles. SIDAR array was mounted in C208800800024 lampshade configuration at backward angles to cover C208800800025 angles between 135deg and 165deg. C208800800026 ERR-ANALYS (ERR-4) Syst. uncertainty in sieve rate C208800800027 (ERR-5) Syst. uncert. in normalization run statistics C208800800028 (ERR-6) Systematic uncertainty in normalization gating C208800800029 (ERR-T) Total uncertainty C208800800030 (ERR-S) Combined uncertainty from counting statistics C208800800031 and Gaussian fits of binned angular data C208800800032 ENDBIB 30 0 C208800800033 COMMON 5 3 C208800800034 EN ERR-4 ERR-5 ERR-6 ERR-T C208800800035 MEV PER-CENT PER-CENT PER-CENT PER-CENT C208800800036 18.0 1.0 6.0 5.0 10.0 C208800800037 ENDCOMMON 3 0 C208800800038 DATA 3 12 C208800800039 ANG-CM DATA ERR-S C208800800040 ADEG NO-DIM NO-DIM C208800800041 29.0 5.67 0.19 C208800800042 30.9 3.58 0.22 C208800800043 32.7 2.33 0.26 C208800800044 34.5 1.73 0.30 C208800800045 37.4 0.43 0.20 C208800800046 40.6 0.71 0.16 C208800800047 43.7 1.96 0.22 C208800800048 46.9 3.71 0.23 C208800800049 50.1 4.25 0.27 C208800800050 53.3 4.92 0.33 C208800800051 56.5 3.56 0.23 C208800800052 59.7 3.87 0.59 C208800800053 ENDDATA 14 0 C208800800054 ENDSUBENT 53 0 C208800899999 SUBENT C2088009 20140123 C139C208800900001 BIB 5 30 C208800900002 REACTION (4-BE-10(D,EL)4-BE-10,,DA,,RTH) C208800900003 STATUS (TABLE) Data presented in fig. 3 of the reference takenC208800900004 from tabulated data given in Supplemental Material at C208800900005 http: C208800900006 //link.aps.org/supplemental/10.1103/PhysRevC.88.064612 C208800900007 SAMPLE The CD2 targets were prepared from deuterated C208800900008 polyethylene powder with areal densities of 94, 143, C208800900009 162, and 185 mu-g/cm2. The thickness of each target C208800900010 was measured using the energy loss of 5.805-MeV alpha C208800900011 particles from the decay of 244Cm. C208800900012 DETECTOR (MCPLT) A new dual microchannel plate (DMCP) detector C208800900013 was employed for heavy recoil detection. The DMCP C208800900014 utilizes two conventional MCP detectors viewing C208800900015 opposing sides of a single carbon or metallized foil. C208800900016 (SI) For the data taken with deuterated targets, the C208800900017 angles and energies of light ion ejectiles were C208800900018 measured using the Silicon Detector Array (SIDAR) and C208800900019 the first full implementation of the Oak Ridge C208800900020 Rutgers Barrel Array (ORRUBA). ORRUBA detectors (1000 C208800900021 mu-m thick) were mounted at a radius of 87 mm from C208800900022 the beam axis at theta(lab) > 95 deg and at 76 mm at C208800900023 more forward angles. SIDAR array was mounted in C208800900024 lampshade configuration at backward angles to cover C208800900025 angles between 135deg and 165deg. C208800900026 ERR-ANALYS (ERR-4) Syst. uncertainty in sieve rate C208800900027 (ERR-5) Syst. uncert. in normalization run statistics C208800900028 (ERR-6) Systematic uncertainty in normalization gating C208800900029 (ERR-T) Total uncertainty C208800900030 (ERR-S) Combined uncertainty from counting statistics C208800900031 and Gaussian fits of binned angular data C208800900032 ENDBIB 30 0 C208800900033 COMMON 5 3 C208800900034 EN ERR-4 ERR-5 ERR-6 ERR-T C208800900035 MEV PER-CENT PER-CENT PER-CENT PER-CENT C208800900036 21.4 1.0 4.0 5.0 10.0 C208800900037 ENDCOMMON 3 0 C208800900038 DATA 3 15 C208800900039 ANG-CM DATA ERR-S C208800900040 ADEG NO-DIM NO-DIM C208800900041 30.8 0.18 0.02 C208800900042 32.8 0.36 0.03 C208800900043 34.7 0.82 0.05 C208800900044 36.7 1.85 0.07 C208800900045 38.7 2.94 0.09 C208800900046 40.7 4.17 0.11 C208800900047 42.4 4.86 0.13 C208800900048 44.7 5.90 0.15 C208800900049 46.7 5.91 0.17 C208800900050 48.7 5.88 0.18 C208800900051 50.7 5.47 0.18 C208800900052 52.6 4.42 0.18 C208800900053 54.6 3.51 0.18 C208800900054 56.6 2.81 0.17 C208800900055 58.6 1.20 0.21 C208800900056 ENDDATA 17 0 C208800900057 ENDSUBENT 56 0 C208800999999 SUBENT C2088010 20140123 C139C208801000001 BIB 5 30 C208801000002 REACTION (4-BE-10(D,P)4-BE-11,PAR,DA) C208801000003 STATUS (TABLE) Data presented in fig. 7 of the reference takenC208801000004 from tabulated data given in Supplemental Material at C208801000005 http: C208801000006 //link.aps.org/supplemental/10.1103/PhysRevC.88.064612 C208801000007 SAMPLE The CD2 targets were prepared from deuterated C208801000008 polyethylene powder with areal densities of 94, 143, C208801000009 162, and 185 mu-g/cm2. The thickness of each target C208801000010 was measured using the energy loss of 5.805-MeV alpha C208801000011 particles from the decay of 244Cm. C208801000012 DETECTOR (MCPLT) A new dual microchannel plate (DMCP) detector C208801000013 was employed for heavy recoil detection. The DMCP C208801000014 utilizes two conventional MCP detectors viewing C208801000015 opposing sides of a single carbon or metallized foil. C208801000016 (SI) For the data taken with deuterated targets, the C208801000017 angles and energies of light ion ejectiles were C208801000018 measured using the Silicon Detector Array (SIDAR) and C208801000019 the first full implementation of the Oak Ridge C208801000020 Rutgers Barrel Array (ORRUBA). ORRUBA detectors (1000 C208801000021 mu-m thick) were mounted at a radius of 87 mm from C208801000022 the beam axis at theta(lab) > 95 deg and at 76 mm at C208801000023 more forward angles. SIDAR array was mounted in C208801000024 lampshade configuration at backward angles to cover C208801000025 angles between 135deg and 165deg. C208801000026 ERR-ANALYS (ERR-4) Syst. uncertainty in sieve rate C208801000027 (ERR-5) Syst. uncert. in normalization run statistics C208801000028 (ERR-6) Systematic uncertainty in normalization gating C208801000029 (ERR-T) Total uncertainty C208801000030 (ERR-S) Combined uncertainty from counting statistics C208801000031 and Gaussian fits of binned angular data C208801000032 ENDBIB 30 0 C208801000033 COMMON 6 3 C208801000034 EN E-LVL ERR-4 ERR-5 ERR-6 ERR-T C208801000035 MEV MEV PER-CENT PER-CENT PER-CENT PER-CENT C208801000036 12.0 0.0 1.0 6.0 5.0 11.0 C208801000037 ENDCOMMON 3 0 C208801000038 DATA 3 11 C208801000039 ANG-CM DATA-CM ERR-S C208801000040 ADEG MB/SR MB/SR C208801000041 4.3 52.4 8.1 C208801000042 5.6 55.0 7.8 C208801000043 7.0 46.4 3.0 C208801000044 8.6 50.9 5.5 C208801000045 10.4 38.8 2.2 C208801000046 53.0 4.09 0.52 C208801000047 56.8 2.31 0.26 C208801000048 60.9 1.92 0.27 C208801000049 65.1 1.57 0.21 C208801000050 69.5 0.95 0.18 C208801000051 74.0 0.64 0.24 C208801000052 ENDDATA 13 0 C208801000053 ENDSUBENT 52 0 C208801099999 SUBENT C2088011 20140123 C139C208801100001 BIB 5 30 C208801100002 REACTION (4-BE-10(D,P)4-BE-11,PAR,DA) C208801100003 STATUS (TABLE) Data presented in fig. 7 of the reference takenC208801100004 from tabulated data given in Supplemental Material at C208801100005 http: C208801100006 //link.aps.org/supplemental/10.1103/PhysRevC.88.064612 C208801100007 SAMPLE The CD2 targets were prepared from deuterated C208801100008 polyethylene powder with areal densities of 94, 143, C208801100009 162, and 185 mu-g/cm2. The thickness of each target C208801100010 was measured using the energy loss of 5.805-MeV alpha C208801100011 particles from the decay of 244Cm. C208801100012 DETECTOR (MCPLT) A new dual microchannel plate (DMCP) detector C208801100013 was employed for heavy recoil detection. The DMCP C208801100014 utilizes two conventional MCP detectors viewing C208801100015 opposing sides of a single carbon or metallized foil. C208801100016 (SI) For the data taken with deuterated targets, the C208801100017 angles and energies of light ion ejectiles were C208801100018 measured using the Silicon Detector Array (SIDAR) and C208801100019 the first full implementation of the Oak Ridge C208801100020 Rutgers Barrel Array (ORRUBA). ORRUBA detectors (1000 C208801100021 mu-m thick) were mounted at a radius of 87 mm from C208801100022 the beam axis at theta(lab) > 95 deg and at 76 mm at C208801100023 more forward angles. SIDAR array was mounted in C208801100024 lampshade configuration at backward angles to cover C208801100025 angles between 135deg and 165deg. C208801100026 ERR-ANALYS (ERR-4) Syst. uncertainty in sieve rate C208801100027 (ERR-5) Syst. uncert. in normalization run statistics C208801100028 (ERR-6) Systematic uncertainty in normalization gating C208801100029 (ERR-T) Total uncertainty C208801100030 (ERR-S) Combined uncertainty from counting statistics C208801100031 and Gaussian fits of binned angular data C208801100032 ENDBIB 30 0 C208801100033 COMMON 6 3 C208801100034 EN E-LVL ERR-4 ERR-5 ERR-6 ERR-T C208801100035 MEV MEV PER-CENT PER-CENT PER-CENT PER-CENT C208801100036 15.0 0.0 1.0 6.0 5.0 10.0 C208801100037 ENDCOMMON 3 0 C208801100038 DATA 3 9 C208801100039 ANG-CM DATA-CM ERR-S C208801100040 ADEG MB/SR MB/SR C208801100041 4.6 41.7 3.2 C208801100042 5.9 37.4 2.7 C208801100043 7.4 33.4 2.4 C208801100044 9.1 25.3 1.8 C208801100045 11.0 17.9 1.3 C208801100046 58.0 4.17 0.69 C208801100047 62.0 2.99 0.40 C208801100048 66.1 1.49 0.37 C208801100049 70.5 0.27 0.23 C208801100050 ENDDATA 11 0 C208801100051 ENDSUBENT 50 0 C208801199999 SUBENT C2088012 20140123 C139C208801200001 BIB 5 30 C208801200002 REACTION (4-BE-10(D,P)4-BE-11,PAR,DA) C208801200003 STATUS (TABLE) Data presented in fig. 7 of the reference takenC208801200004 from tabulated data given in Supplemental Material at C208801200005 http: C208801200006 //link.aps.org/supplemental/10.1103/PhysRevC.88.064612 C208801200007 SAMPLE The CD2 targets were prepared from deuterated C208801200008 polyethylene powder with areal densities of 94, 143, C208801200009 162, and 185 mu-g/cm2. The thickness of each target C208801200010 was measured using the energy loss of 5.805-MeV alpha C208801200011 particles from the decay of 244Cm. C208801200012 DETECTOR (MCPLT) A new dual microchannel plate (DMCP) detector C208801200013 was employed for heavy recoil detection. The DMCP C208801200014 utilizes two conventional MCP detectors viewing C208801200015 opposing sides of a single carbon or metallized foil. C208801200016 (SI) For the data taken with deuterated targets, the C208801200017 angles and energies of light ion ejectiles were C208801200018 measured using the Silicon Detector Array (SIDAR) and C208801200019 the first full implementation of the Oak Ridge C208801200020 Rutgers Barrel Array (ORRUBA). ORRUBA detectors (1000 C208801200021 mu-m thick) were mounted at a radius of 87 mm from C208801200022 the beam axis at theta(lab) > 95 deg and at 76 mm at C208801200023 more forward angles. SIDAR array was mounted in C208801200024 lampshade configuration at backward angles to cover C208801200025 angles between 135deg and 165deg. C208801200026 ERR-ANALYS (ERR-4) Syst. uncertainty in sieve rate C208801200027 (ERR-5) Syst. uncert. in normalization run statistics C208801200028 (ERR-6) Systematic uncertainty in normalization gating C208801200029 (ERR-T) Total uncertainty C208801200030 (ERR-S) Combined uncertainty from counting statistics C208801200031 and Gaussian fits of binned angular data C208801200032 ENDBIB 30 0 C208801200033 COMMON 6 3 C208801200034 EN E-LVL ERR-4 ERR-5 ERR-6 ERR-T C208801200035 MEV MEV PER-CENT PER-CENT PER-CENT PER-CENT C208801200036 18.0 0.0 1.0 6.0 5.0 10.0 C208801200037 ENDCOMMON 3 0 C208801200038 DATA 3 8 C208801200039 ANG-CM DATA-CM ERR-S C208801200040 ADEG MB/SR MB/SR C208801200041 4.7 22.2 1.9 C208801200042 6.1 17.8 1.5 C208801200043 7.6 13.0 1.1 C208801200044 9.4 10.8 0.9 C208801200045 11.3 8.13 0.69 C208801200046 53.0 0.78 0.22 C208801200047 60.7 0.74 0.17 C208801200048 69.0 0.23 0.11 C208801200049 ENDDATA 10 0 C208801200050 ENDSUBENT 49 0 C208801299999 SUBENT C2088013 20140123 C139C208801300001 BIB 5 30 C208801300002 REACTION (4-BE-10(D,P)4-BE-11,PAR,DA) C208801300003 STATUS (TABLE) Data presented in fig. 7 of the reference takenC208801300004 from tabulated data given in Supplemental Material at C208801300005 http: C208801300006 //link.aps.org/supplemental/10.1103/PhysRevC.88.064612 C208801300007 SAMPLE The CD2 targets were prepared from deuterated C208801300008 polyethylene powder with areal densities of 94, 143, C208801300009 162, and 185 mu-g/cm2. The thickness of each target C208801300010 was measured using the energy loss of 5.805-MeV alpha C208801300011 particles from the decay of 244Cm. C208801300012 DETECTOR (MCPLT) A new dual microchannel plate (DMCP) detector C208801300013 was employed for heavy recoil detection. The DMCP C208801300014 utilizes two conventional MCP detectors viewing C208801300015 opposing sides of a single carbon or metallized foil. C208801300016 (SI) For the data taken with deuterated targets, the C208801300017 angles and energies of light ion ejectiles were C208801300018 measured using the Silicon Detector Array (SIDAR) and C208801300019 the first full implementation of the Oak Ridge C208801300020 Rutgers Barrel Array (ORRUBA). ORRUBA detectors (1000 C208801300021 mu-m thick) were mounted at a radius of 87 mm from C208801300022 the beam axis at theta(lab) > 95 deg and at 76 mm at C208801300023 more forward angles. SIDAR array was mounted in C208801300024 lampshade configuration at backward angles to cover C208801300025 angles between 135deg and 165deg. C208801300026 ERR-ANALYS (ERR-4) Syst. uncertainty in sieve rate C208801300027 (ERR-5) Syst. uncert. in normalization run statistics C208801300028 (ERR-6) Systematic uncertainty in normalization gating C208801300029 (ERR-T) Total uncertainty C208801300030 (ERR-S) Combined uncertainty from counting statistics C208801300031 and Gaussian fits of binned angular data C208801300032 ENDBIB 30 0 C208801300033 COMMON 6 3 C208801300034 EN E-LVL ERR-4 ERR-5 ERR-6 ERR-T C208801300035 MEV MEV PER-CENT PER-CENT PER-CENT PER-CENT C208801300036 21.4 0.0 1.0 4.0 5.0 10.0 C208801300037 ENDCOMMON 3 0 C208801300038 DATA 3 15 C208801300039 ANG-CM DATA-CM ERR-S C208801300040 ADEG MB/SR MB/SR C208801300041 4.6 17.52 0.81 C208801300042 5.5 16.18 1.09 C208801300043 6.5 14.78 0.65 C208801300044 7.5 11.93 0.47 C208801300045 8.7 9.26 0.42 C208801300046 9.9 7.55 0.34 C208801300047 11.2 5.44 0.28 C208801300048 12.3 4.28 0.61 C208801300049 18.2 0.85 0.18 C208801300050 20.7 0.13 0.13 C208801300051 23.4 0.68 0.13 C208801300052 26.4 0.81 0.11 C208801300053 29.8 1.21 0.09 C208801300054 33.5 1.19 0.08 C208801300055 37.6 0.65 0.05 C208801300056 ENDDATA 17 0 C208801300057 ENDSUBENT 56 0 C208801399999 SUBENT C2088014 20140123 C139C208801400001 BIB 5 30 C208801400002 REACTION (4-BE-10(D,P)4-BE-11,PAR,DA) C208801400003 STATUS (TABLE) Data presented in fig. 7 of the reference takenC208801400004 from tabulated data given in Supplemental Material at C208801400005 http: C208801400006 //link.aps.org/supplemental/10.1103/PhysRevC.88.064612 C208801400007 SAMPLE The CD2 targets were prepared from deuterated C208801400008 polyethylene powder with areal densities of 94, 143, C208801400009 162, and 185 mu-g/cm2. The thickness of each target C208801400010 was measured using the energy loss of 5.805-MeV alpha C208801400011 particles from the decay of 244Cm. C208801400012 DETECTOR (MCPLT) A new dual microchannel plate (DMCP) detector C208801400013 was employed for heavy recoil detection. The DMCP C208801400014 utilizes two conventional MCP detectors viewing C208801400015 opposing sides of a single carbon or metallized foil. C208801400016 (SI) For the data taken with deuterated targets, the C208801400017 angles and energies of light ion ejectiles were C208801400018 measured using the Silicon Detector Array (SIDAR) and C208801400019 the first full implementation of the Oak Ridge C208801400020 Rutgers Barrel Array (ORRUBA). ORRUBA detectors (1000 C208801400021 mu-m thick) were mounted at a radius of 87 mm from C208801400022 the beam axis at theta(lab) > 95 deg and at 76 mm at C208801400023 more forward angles. SIDAR array was mounted in C208801400024 lampshade configuration at backward angles to cover C208801400025 angles between 135deg and 165deg. C208801400026 ERR-ANALYS (ERR-4) Syst. uncertainty in sieve rate C208801400027 (ERR-5) Syst. uncert. in normalization run statistics C208801400028 (ERR-6) Systematic uncertainty in normalization gating C208801400029 (ERR-T) Total uncertainty C208801400030 (ERR-S) Combined uncertainty from counting statistics C208801400031 and Gaussian fits of binned angular data C208801400032 ENDBIB 30 0 C208801400033 COMMON 6 3 C208801400034 EN E-LVL ERR-4 ERR-5 ERR-6 ERR-T C208801400035 MEV MEV PER-CENT PER-CENT PER-CENT PER-CENT C208801400036 12.0 0.32 1.0 6.0 5.0 11.0 C208801400037 ENDCOMMON 3 0 C208801400038 DATA 3 12 C208801400039 ANG-CM DATA-CM ERR-S C208801400040 ADEG MB/SR MB/SR C208801400041 4.1 42.6 5.0 C208801400042 5.3 34.9 5.2 C208801400043 6.6 37.4 2.2 C208801400044 8.1 38.4 4.2 C208801400045 9.9 44.0 2.8 C208801400046 51.8 5.41 0.61 C208801400047 55.7 4.45 0.33 C208801400048 59.7 3.91 0.34 C208801400049 64.0 3.43 0.27 C208801400050 68.4 2.65 0.24 C208801400051 73.0 2.02 0.32 C208801400052 77.7 1.50 0.34 C208801400053 ENDDATA 14 0 C208801400054 ENDSUBENT 53 0 C208801499999 SUBENT C2088015 20140123 C139C208801500001 BIB 5 30 C208801500002 REACTION (4-BE-10(D,P)4-BE-11,PAR,DA) C208801500003 STATUS (TABLE) Data presented in fig. 7 of the reference takenC208801500004 from tabulated data given in Supplemental Material at C208801500005 http: C208801500006 //link.aps.org/supplemental/10.1103/PhysRevC.88.064612 C208801500007 SAMPLE The CD2 targets were prepared from deuterated C208801500008 polyethylene powder with areal densities of 94, 143, C208801500009 162, and 185 mu-g/cm2. The thickness of each target C208801500010 was measured using the energy loss of 5.805-MeV alpha C208801500011 particles from the decay of 244Cm. C208801500012 DETECTOR (MCPLT) A new dual microchannel plate (DMCP) detector C208801500013 was employed for heavy recoil detection. The DMCP C208801500014 utilizes two conventional MCP detectors viewing C208801500015 opposing sides of a single carbon or metallized foil. C208801500016 (SI) For the data taken with deuterated targets, the C208801500017 angles and energies of light ion ejectiles were C208801500018 measured using the Silicon Detector Array (SIDAR) and C208801500019 the first full implementation of the Oak Ridge C208801500020 Rutgers Barrel Array (ORRUBA). ORRUBA detectors (1000 C208801500021 mu-m thick) were mounted at a radius of 87 mm from C208801500022 the beam axis at theta(lab) > 95 deg and at 76 mm at C208801500023 more forward angles. SIDAR array was mounted in C208801500024 lampshade configuration at backward angles to cover C208801500025 angles between 135deg and 165deg. C208801500026 ERR-ANALYS (ERR-4) Syst. uncertainty in sieve rate C208801500027 (ERR-5) Syst. uncert. in normalization run statistics C208801500028 (ERR-6) Systematic uncertainty in normalization gating C208801500029 (ERR-T) Total uncertainty C208801500030 (ERR-S) Combined uncertainty from counting statistics C208801500031 and Gaussian fits of binned angular data C208801500032 ENDBIB 30 0 C208801500033 COMMON 6 3 C208801500034 EN E-LVL ERR-4 ERR-5 ERR-6 ERR-T C208801500035 MEV MEV PER-CENT PER-CENT PER-CENT PER-CENT C208801500036 15.0 0.32 1.0 6.0 5.0 10.0 C208801500037 ENDCOMMON 3 0 C208801500038 DATA 3 9 C208801500039 ANG-CM DATA-CM ERR-S C208801500040 ADEG MB/SR MB/SR C208801500041 4.4 34.3 2.7 C208801500042 5.7 33.2 2.5 C208801500043 7.1 32.4 2.4 C208801500044 8.7 28.3 2.0 C208801500045 10.6 25.3 1.8 C208801500046 57.1 4.85 0.75 C208801500047 61.1 4.48 0.46 C208801500048 65.3 3.22 0.48 C208801500049 69.7 2.18 0.35 C208801500050 ENDDATA 11 0 C208801500051 ENDSUBENT 50 0 C208801599999 SUBENT C2088016 20140123 C139C208801600001 BIB 5 30 C208801600002 REACTION (4-BE-10(D,P)4-BE-11,PAR,DA) C208801600003 STATUS (TABLE) Data presented in fig. 7 of the reference takenC208801600004 from tabulated data given in Supplemental Material at C208801600005 http: C208801600006 //link.aps.org/supplemental/10.1103/PhysRevC.88.064612 C208801600007 SAMPLE The CD2 targets were prepared from deuterated C208801600008 polyethylene powder with areal densities of 94, 143, C208801600009 162, and 185 mu-g/cm2. The thickness of each target C208801600010 was measured using the energy loss of 5.805-MeV alpha C208801600011 particles from the decay of 244Cm. C208801600012 DETECTOR (MCPLT) A new dual microchannel plate (DMCP) detector C208801600013 was employed for heavy recoil detection. The DMCP C208801600014 utilizes two conventional MCP detectors viewing C208801600015 opposing sides of a single carbon or metallized foil. C208801600016 (SI) For the data taken with deuterated targets, the C208801600017 angles and energies of light ion ejectiles were C208801600018 measured using the Silicon Detector Array (SIDAR) and C208801600019 the first full implementation of the Oak Ridge C208801600020 Rutgers Barrel Array (ORRUBA). ORRUBA detectors (1000 C208801600021 mu-m thick) were mounted at a radius of 87 mm from C208801600022 the beam axis at theta(lab) > 95 deg and at 76 mm at C208801600023 more forward angles. SIDAR array was mounted in C208801600024 lampshade configuration at backward angles to cover C208801600025 angles between 135deg and 165deg. C208801600026 ERR-ANALYS (ERR-4) Syst. uncertainty in sieve rate C208801600027 (ERR-5) Syst. uncert. in normalization run statistics C208801600028 (ERR-6) Systematic uncertainty in normalization gating C208801600029 (ERR-T) Total uncertainty C208801600030 (ERR-S) Combined uncertainty from counting statistics C208801600031 and Gaussian fits of binned angular data C208801600032 ENDBIB 30 0 C208801600033 COMMON 6 3 C208801600034 EN E-LVL ERR-4 ERR-5 ERR-6 ERR-T C208801600035 MEV MEV PER-CENT PER-CENT PER-CENT PER-CENT C208801600036 18.0 0.32 1.0 6.0 5.0 10.0 C208801600037 ENDCOMMON 3 0 C208801600038 DATA 3 8 C208801600039 ANG-CM DATA-CM ERR-S C208801600040 ADEG MB/SR MB/SR C208801600041 4.6 20.4 1.8 C208801600042 5.9 18.6 1.5 C208801600043 7.4 17.9 1.5 C208801600044 9.1 15.6 1.2 C208801600045 11.0 14.6 1.2 C208801600046 52.3 1.34 0.28 C208801600047 60.0 0.85 0.18 C208801600048 68.3 0.37 0.13 C208801600049 ENDDATA 10 0 C208801600050 ENDSUBENT 49 0 C208801699999 SUBENT C2088017 20140123 C139C208801700001 BIB 5 30 C208801700002 REACTION (4-BE-10(D,P)4-BE-11,PAR,DA) C208801700003 STATUS (TABLE) Data presented in fig. 7 of the reference takenC208801700004 from tabulated data given in Supplemental Material at C208801700005 http: C208801700006 //link.aps.org/supplemental/10.1103/PhysRevC.88.064612 C208801700007 SAMPLE The CD2 targets were prepared from deuterated C208801700008 polyethylene powder with areal densities of 94, 143, C208801700009 162, and 185 mu-g/cm2. The thickness of each target C208801700010 was measured using the energy loss of 5.805-MeV alpha C208801700011 particles from the decay of 244Cm. C208801700012 DETECTOR (MCPLT) A new dual microchannel plate (DMCP) detector C208801700013 was employed for heavy recoil detection. The DMCP C208801700014 utilizes two conventional MCP detectors viewing C208801700015 opposing sides of a single carbon or metallized foil. C208801700016 (SI) For the data taken with deuterated targets, the C208801700017 angles and energies of light ion ejectiles were C208801700018 measured using the Silicon Detector Array (SIDAR) and C208801700019 the first full implementation of the Oak Ridge C208801700020 Rutgers Barrel Array (ORRUBA). ORRUBA detectors (1000 C208801700021 mu-m thick) were mounted at a radius of 87 mm from C208801700022 the beam axis at theta(lab) > 95 deg and at 76 mm at C208801700023 more forward angles. SIDAR array was mounted in C208801700024 lampshade configuration at backward angles to cover C208801700025 angles between 135deg and 165deg. C208801700026 ERR-ANALYS (ERR-4) Syst. uncertainty in sieve rate C208801700027 (ERR-5) Syst. uncert. in normalization run statistics C208801700028 (ERR-6) Systematic uncertainty in normalization gating C208801700029 (ERR-T) Total uncertainty C208801700030 (ERR-S) Combined uncertainty from counting statistics C208801700031 and Gaussian fits of binned angular data C208801700032 ENDBIB 30 0 C208801700033 COMMON 6 3 C208801700034 EN E-LVL ERR-4 ERR-5 ERR-6 ERR-T C208801700035 MEV MEV PER-CENT PER-CENT PER-CENT PER-CENT C208801700036 21.4 0.32 1.0 4.0 5.0 10.0 C208801700037 ENDCOMMON 3 0 C208801700038 DATA 3 15 C208801700039 ANG-CM DATA-CM ERR-S C208801700040 ADEG MB/SR MB/SR C208801700041 4.5 20.6 1.9 C208801700042 5.4 19.5 2.0 C208801700043 6.3 20.0 1.8 C208801700044 7.4 18.8 1.6 C208801700045 8.5 17.4 1.5 C208801700046 9.7 15.2 1.3 C208801700047 11.0 13.8 1.1 C208801700048 12.0 13.0 1.3 C208801700049 17.8 9.14 0.78 C208801700050 20.2 6.93 0.60 C208801700051 22.9 5.23 0.45 C208801700052 25.9 3.78 0.33 C208801700053 29.2 2.61 0.23 C208801700054 32.9 2.23 0.20 C208801700055 37.0 2.16 0.19 C208801700056 ENDDATA 17 0 C208801700057 ENDSUBENT 56 0 C208801799999 SUBENT C2088018 20140123 C139C208801800001 BIB 5 30 C208801800002 REACTION (4-BE-10(D,P)4-BE-11,PAR,DA) C208801800003 STATUS (TABLE) Data presented in fig. 8 of the reference takenC208801800004 from tabulated data given in Supplemental Material at C208801800005 http: C208801800006 //link.aps.org/supplemental/10.1103/PhysRevC.88.064612 C208801800007 SAMPLE The CD2 targets were prepared from deuterated C208801800008 polyethylene powder with areal densities of 94, 143, C208801800009 162, and 185 mu-g/cm2. The thickness of each target C208801800010 was measured using the energy loss of 5.805-MeV alpha C208801800011 particles from the decay of 244Cm. C208801800012 DETECTOR (MCPLT) A new dual microchannel plate (DMCP) detector C208801800013 was employed for heavy recoil detection. The DMCP C208801800014 utilizes two conventional MCP detectors viewing C208801800015 opposing sides of a single carbon or metallized foil. C208801800016 (SI) For the data taken with deuterated targets, the C208801800017 angles and energies of light ion ejectiles were C208801800018 measured using the Silicon Detector Array (SIDAR) and C208801800019 the first full implementation of the Oak Ridge C208801800020 Rutgers Barrel Array (ORRUBA). ORRUBA detectors (1000 C208801800021 mu-m thick) were mounted at a radius of 87 mm from C208801800022 the beam axis at theta(lab) > 95 deg and at 76 mm at C208801800023 more forward angles. SIDAR array was mounted in C208801800024 lampshade configuration at backward angles to cover C208801800025 angles between 135deg and 165deg. C208801800026 ERR-ANALYS (ERR-4) Syst. uncertainty in sieve rate C208801800027 (ERR-5) Syst. uncert. in normalization run statistics C208801800028 (ERR-6) Systematic uncertainty in normalization gating C208801800029 (ERR-T) Total uncertainty C208801800030 (ERR-S) Combined uncertainty from counting statistics C208801800031 and Gaussian fits of binned angular data C208801800032 ENDBIB 30 0 C208801800033 COMMON 6 3 C208801800034 EN E-LVL ERR-4 ERR-5 ERR-6 ERR-T C208801800035 MEV MEV PER-CENT PER-CENT PER-CENT PER-CENT C208801800036 15.0 1.78 1.0 6.0 5.0 10.0 C208801800037 ENDCOMMON 3 0 C208801800038 DATA 3 9 C208801800039 ANG-CM DATA-CM ERR-S C208801800040 ADEG MB/SR MB/SR C208801800041 4.5 72.0 14.0 C208801800042 5.6 106.0 16.0 C208801800043 6.9 64.8 9.4 C208801800044 8.4 52.7 7.2 C208801800045 48.4 11.1 0.9 C208801800046 52.3 7.36 0.74 C208801800047 56.5 9.24 0.76 C208801800048 60.9 8.05 0.76 C208801800049 65.5 9.43 0.74 C208801800050 ENDDATA 11 0 C208801800051 ENDSUBENT 50 0 C208801899999 SUBENT C2088019 20140123 C139C208801900001 BIB 5 30 C208801900002 REACTION (4-BE-10(D,P)4-BE-11,PAR,DA) C208801900003 STATUS (TABLE) Data presented in fig. 8 of the reference takenC208801900004 from tabulated data given in Supplemental Material at C208801900005 http: C208801900006 //link.aps.org/supplemental/10.1103/PhysRevC.88.064612 C208801900007 SAMPLE The CD2 targets were prepared from deuterated C208801900008 polyethylene powder with areal densities of 94, 143, C208801900009 162, and 185 mu-g/cm2. The thickness of each target C208801900010 was measured using the energy loss of 5.805-MeV alpha C208801900011 particles from the decay of 244Cm. C208801900012 DETECTOR (MCPLT) A new dual microchannel plate (DMCP) detector C208801900013 was employed for heavy recoil detection. The DMCP C208801900014 utilizes two conventional MCP detectors viewing C208801900015 opposing sides of a single carbon or metallized foil. C208801900016 (SI) For the data taken with deuterated targets, the C208801900017 angles and energies of light ion ejectiles were C208801900018 measured using the Silicon Detector Array (SIDAR) and C208801900019 the first full implementation of the Oak Ridge C208801900020 Rutgers Barrel Array (ORRUBA). ORRUBA detectors (1000 C208801900021 mu-m thick) were mounted at a radius of 87 mm from C208801900022 the beam axis at theta(lab) > 95 deg and at 76 mm at C208801900023 more forward angles. SIDAR array was mounted in C208801900024 lampshade configuration at backward angles to cover C208801900025 angles between 135deg and 165deg. C208801900026 ERR-ANALYS (ERR-4) Syst. uncertainty in sieve rate C208801900027 (ERR-5) Syst. uncert. in normalization run statistics C208801900028 (ERR-6) Systematic uncertainty in normalization gating C208801900029 (ERR-T) Total uncertainty C208801900030 (ERR-S) Combined uncertainty from counting statistics C208801900031 and Gaussian fits of binned angular data C208801900032 ENDBIB 30 0 C208801900033 COMMON 6 3 C208801900034 EN E-LVL ERR-4 ERR-5 ERR-6 ERR-T C208801900035 MEV MEV PER-CENT PER-CENT PER-CENT PER-CENT C208801900036 18.0 1.78 1.0 6.0 5.0 10.0 C208801900037 ENDCOMMON 3 0 C208801900038 DATA 3 9 C208801900039 ANG-CM DATA-CM ERR-S C208801900040 ADEG MB/SR MB/SR C208801900041 3.8 63.7 5.4 C208801900042 5.0 68.5 6.2 C208801900043 6.2 49.8 4.3 C208801900044 7.7 50.0 4.0 C208801900045 9.3 50.2 4.3 C208801900046 48.6 1.63 0.47 C208801900047 56.5 1.28 0.22 C208801900048 65.1 1.87 0.28 C208801900049 71.8 1.85 0.30 C208801900050 ENDDATA 11 0 C208801900051 ENDSUBENT 50 0 C208801999999 SUBENT C2088020 20140123 C139C208802000001 BIB 5 30 C208802000002 REACTION (4-BE-10(D,P)4-BE-11,PAR,DA) C208802000003 STATUS (TABLE) Data presented in fig. 8 of the reference takenC208802000004 from tabulated data given in Supplemental Material at C208802000005 http: C208802000006 //link.aps.org/supplemental/10.1103/PhysRevC.88.064612 C208802000007 SAMPLE The CD2 targets were prepared from deuterated C208802000008 polyethylene powder with areal densities of 94, 143, C208802000009 162, and 185 mu-g/cm2. The thickness of each target C208802000010 was measured using the energy loss of 5.805-MeV alpha C208802000011 particles from the decay of 244Cm. C208802000012 DETECTOR (MCPLT) A new dual microchannel plate (DMCP) detector C208802000013 was employed for heavy recoil detection. The DMCP C208802000014 utilizes two conventional MCP detectors viewing C208802000015 opposing sides of a single carbon or metallized foil. C208802000016 (SI) For the data taken with deuterated targets, the C208802000017 angles and energies of light ion ejectiles were C208802000018 measured using the Silicon Detector Array (SIDAR) and C208802000019 the first full implementation of the Oak Ridge C208802000020 Rutgers Barrel Array (ORRUBA). ORRUBA detectors (1000 C208802000021 mu-m thick) were mounted at a radius of 87 mm from C208802000022 the beam axis at theta(lab) > 95 deg and at 76 mm at C208802000023 more forward angles. SIDAR array was mounted in C208802000024 lampshade configuration at backward angles to cover C208802000025 angles between 135deg and 165deg. C208802000026 ERR-ANALYS (ERR-4) Syst. uncertainty in sieve rate C208802000027 (ERR-5) Syst. uncert. in normalization run statistics C208802000028 (ERR-6) Systematic uncertainty in normalization gating C208802000029 (ERR-T) Total uncertainty C208802000030 (ERR-S) Combined uncertainty from counting statistics C208802000031 and Gaussian fits of binned angular data C208802000032 ENDBIB 30 0 C208802000033 COMMON 6 3 C208802000034 EN E-LVL ERR-4 ERR-5 ERR-6 ERR-T C208802000035 MEV MEV PER-CENT PER-CENT PER-CENT PER-CENT C208802000036 21.4 1.78 1.0 4.0 5.0 10.0 C208802000037 ENDCOMMON 3 0 C208802000038 DATA 3 15 C208802000039 ANG-CM DATA-CM ERR-S C208802000040 ADEG MB/SR MB/SR C208802000041 3.9 92.0 7.5 C208802000042 4.7 92.5 7.5 C208802000043 5.6 86.6 7.0 C208802000044 6.5 84.3 6.8 C208802000045 7.4 79.0 6.4 C208802000046 8.5 72.5 5.9 C208802000047 9.7 67.3 5.4 C208802000048 10.6 67.5 5.5 C208802000049 15.8 43.2 3.5 C208802000050 18.1 35.5 2.9 C208802000051 20.6 27.1 2.2 C208802000052 23.4 19.2 1.6 C208802000053 26.6 12.7 1.0 C208802000054 30.1 7.05 0.57 C208802000055 34.1 2.92 0.24 C208802000056 ENDDATA 17 0 C208802000057 ENDSUBENT 56 0 C208802099999 SUBENT C2088021 20140123 C139C208802100001 BIB 5 30 C208802100002 REACTION (4-BE-10(D,INL)4-BE-10,PAR,DA,,RTH) C208802100003 STATUS (TABLE) Data presented in fig. 4 of the reference takenC208802100004 from tabulated data given in Supplemental Material at C208802100005 http: C208802100006 //link.aps.org/supplemental/10.1103/PhysRevC.88.064612 C208802100007 SAMPLE The CD2 targets were prepared from deuterated C208802100008 polyethylene powder with areal densities of 94, 143, C208802100009 162, and 185 mu-g/cm2. The thickness of each target C208802100010 was measured using the energy loss of 5.805-MeV alpha C208802100011 particles from the decay of 244Cm. C208802100012 DETECTOR (MCPLT) A new dual microchannel plate (DMCP) detector C208802100013 was employed for heavy recoil detection. The DMCP C208802100014 utilizes two conventional MCP detectors viewing C208802100015 opposing sides of a single carbon or metallized foil. C208802100016 (SI) For the data taken with deuterated targets, the C208802100017 angles and energies of light ion ejectiles were C208802100018 measured using the Silicon Detector Array (SIDAR) and C208802100019 the first full implementation of the Oak Ridge C208802100020 Rutgers Barrel Array (ORRUBA). ORRUBA detectors (1000 C208802100021 mu-m thick) were mounted at a radius of 87 mm from C208802100022 the beam axis at theta(lab) > 95 deg and at 76 mm at C208802100023 more forward angles. SIDAR array was mounted in C208802100024 lampshade configuration at backward angles to cover C208802100025 angles between 135deg and 165deg. C208802100026 ERR-ANALYS (ERR-4) Syst. uncertainty in sieve rate C208802100027 (ERR-5) Syst. uncert. in normalization run statistics C208802100028 (ERR-6) Systematic uncertainty in normalization gating C208802100029 (ERR-T) Total uncertainty C208802100030 (ERR-S) Combined uncertainty from counting statistics C208802100031 and Gaussian fits of binned angular data C208802100032 ENDBIB 30 0 C208802100033 COMMON 6 3 C208802100034 EN E-LVL ERR-4 ERR-5 ERR-6 ERR-T C208802100035 MEV MEV PER-CENT PER-CENT PER-CENT PER-CENT C208802100036 12.0 3.368 1.0 6.0 5.0 11.0 C208802100037 ENDCOMMON 3 0 C208802100038 DATA 3 4 C208802100039 ANG-CM DATA ERR-S C208802100040 ADEG NO-DIM NO-DIM C208802100041 36.4 21.9 0.9 C208802100042 41.9 12.7 0.7 C208802100043 46.9 9.41 0.57 C208802100044 51.6 9.17 0.56 C208802100045 ENDDATA 6 0 C208802100046 ENDSUBENT 45 0 C208802199999 SUBENT C2088022 20140123 C139C208802200001 BIB 5 30 C208802200002 REACTION (4-BE-10(D,INL)4-BE-10,PAR,DA,,RTH) C208802200003 STATUS (TABLE) Data presented in fig. 4 of the reference takenC208802200004 from tabulated data given in Supplemental Material at C208802200005 http: C208802200006 //link.aps.org/supplemental/10.1103/PhysRevC.88.064612 C208802200007 SAMPLE The CD2 targets were prepared from deuterated C208802200008 polyethylene powder with areal densities of 94, 143, C208802200009 162, and 185 mu-g/cm2. The thickness of each target C208802200010 was measured using the energy loss of 5.805-MeV alpha C208802200011 particles from the decay of 244Cm. C208802200012 DETECTOR (MCPLT) A new dual microchannel plate (DMCP) detector C208802200013 was employed for heavy recoil detection. The DMCP C208802200014 utilizes two conventional MCP detectors viewing C208802200015 opposing sides of a single carbon or metallized foil. C208802200016 (SI) For the data taken with deuterated targets, the C208802200017 angles and energies of light ion ejectiles were C208802200018 measured using the Silicon Detector Array (SIDAR) and C208802200019 the first full implementation of the Oak Ridge C208802200020 Rutgers Barrel Array (ORRUBA). ORRUBA detectors (1000 C208802200021 mu-m thick) were mounted at a radius of 87 mm from C208802200022 the beam axis at theta(lab) > 95 deg and at 76 mm at C208802200023 more forward angles. SIDAR array was mounted in C208802200024 lampshade configuration at backward angles to cover C208802200025 angles between 135deg and 165deg. C208802200026 ERR-ANALYS (ERR-4) Syst. uncertainty in sieve rate C208802200027 (ERR-5) Syst. uncert. in normalization run statistics C208802200028 (ERR-6) Systematic uncertainty in normalization gating C208802200029 (ERR-T) Total uncertainty C208802200030 (ERR-S) Combined uncertainty from counting statistics C208802200031 and Gaussian fits of binned angular data C208802200032 ENDBIB 30 0 C208802200033 COMMON 6 3 C208802200034 EN E-LVL ERR-4 ERR-5 ERR-6 ERR-T C208802200035 MEV MEV PER-CENT PER-CENT PER-CENT PER-CENT C208802200036 15.0 3.368 1.0 6.0 5.0 10.0 C208802200037 ENDCOMMON 3 0 C208802200038 DATA 3 6 C208802200039 ANG-CM DATA ERR-S C208802200040 ADEG NO-DIM NO-DIM C208802200041 41.0 11.8 0.4 C208802200042 45.0 9.70 0.35 C208802200043 48.7 8.63 0.33 C208802200044 52.2 7.58 0.31 C208802200045 55.5 6.77 0.29 C208802200046 58.7 6.27 0.28 C208802200047 ENDDATA 8 0 C208802200048 ENDSUBENT 47 0 C208802299999 SUBENT C2088023 20140123 C139C208802300001 BIB 5 30 C208802300002 REACTION (4-BE-10(D,INL)4-BE-10,PAR,DA,,RTH) C208802300003 STATUS (TABLE) Data presented in fig. 4 of the reference takenC208802300004 from tabulated data given in Supplemental Material at C208802300005 http: C208802300006 //link.aps.org/supplemental/10.1103/PhysRevC.88.064612 C208802300007 SAMPLE The CD2 targets were prepared from deuterated C208802300008 polyethylene powder with areal densities of 94, 143, C208802300009 162, and 185 mu-g/cm2. The thickness of each target C208802300010 was measured using the energy loss of 5.805-MeV alpha C208802300011 particles from the decay of 244Cm. C208802300012 DETECTOR (MCPLT) A new dual microchannel plate (DMCP) detector C208802300013 was employed for heavy recoil detection. The DMCP C208802300014 utilizes two conventional MCP detectors viewing C208802300015 opposing sides of a single carbon or metallized foil. C208802300016 (SI) For the data taken with deuterated targets, the C208802300017 angles and energies of light ion ejectiles were C208802300018 measured using the Silicon Detector Array (SIDAR) and C208802300019 the first full implementation of the Oak Ridge C208802300020 Rutgers Barrel Array (ORRUBA). ORRUBA detectors (1000 C208802300021 mu-m thick) were mounted at a radius of 87 mm from C208802300022 the beam axis at theta(lab) > 95 deg and at 76 mm at C208802300023 more forward angles. SIDAR array was mounted in C208802300024 lampshade configuration at backward angles to cover C208802300025 angles between 135deg and 165deg. C208802300026 ERR-ANALYS (ERR-4) Syst. uncertainty in sieve rate C208802300027 (ERR-5) Syst. uncert. in normalization run statistics C208802300028 (ERR-6) Systematic uncertainty in normalization gating C208802300029 (ERR-T) Total uncertainty C208802300030 (ERR-S) Combined uncertainty from counting statistics C208802300031 and Gaussian fits of binned angular data C208802300032 ENDBIB 30 0 C208802300033 COMMON 6 3 C208802300034 EN E-LVL ERR-4 ERR-5 ERR-6 ERR-T C208802300035 MEV MEV PER-CENT PER-CENT PER-CENT PER-CENT C208802300036 18.0 3.368 1.0 6.0 5.0 10.0 C208802300037 ENDCOMMON 3 0 C208802300038 DATA 3 7 C208802300039 ANG-CM DATA ERR-S C208802300040 ADEG NO-DIM NO-DIM C208802300041 36.9 8.74 0.51 C208802300042 40.4 11.0 0.6 C208802300043 43.7 8.41 0.50 C208802300044 46.7 6.52 0.44 C208802300045 49.6 5.85 0.42 C208802300046 52.4 5.29 0.39 C208802300047 55.1 6.15 0.43 C208802300048 ENDDATA 9 0 C208802300049 ENDSUBENT 48 0 C208802399999 SUBENT C2088024 20140123 C139C208802400001 BIB 5 30 C208802400002 REACTION (4-BE-10(D,INL)4-BE-10,PAR,DA,,RTH) C208802400003 STATUS (TABLE) Data presented in fig. 3 of the reference takenC208802400004 from tabulated data given in Supplemental Material at C208802400005 http: C208802400006 //link.aps.org/supplemental/10.1103/PhysRevC.88.064612 C208802400007 SAMPLE The CD2 targets were prepared from deuterated C208802400008 polyethylene powder with areal densities of 94, 143, C208802400009 162, and 185 mu-g/cm2. The thickness of each target C208802400010 was measured using the energy loss of 5.805-MeV alpha C208802400011 particles from the decay of 244Cm. C208802400012 DETECTOR (MCPLT) A new dual microchannel plate (DMCP) detector C208802400013 was employed for heavy recoil detection. The DMCP C208802400014 utilizes two conventional MCP detectors viewing C208802400015 opposing sides of a single carbon or metallized foil. C208802400016 (SI) For the data taken with deuterated targets, the C208802400017 angles and energies of light ion ejectiles were C208802400018 measured using the Silicon Detector Array (SIDAR) and C208802400019 the first full implementation of the Oak Ridge C208802400020 Rutgers Barrel Array (ORRUBA). ORRUBA detectors (1000 C208802400021 mu-m thick) were mounted at a radius of 87 mm from C208802400022 the beam axis at theta(lab) > 95 deg and at 76 mm at C208802400023 more forward angles. SIDAR array was mounted in C208802400024 lampshade configuration at backward angles to cover C208802400025 angles between 135deg and 165deg. C208802400026 ERR-ANALYS (ERR-4) Syst. uncertainty in sieve rate C208802400027 (ERR-5) Syst. uncert. in normalization run statistics C208802400028 (ERR-6) Systematic uncertainty in normalization gating C208802400029 (ERR-T) Total uncertainty C208802400030 (ERR-S) Combined uncertainty from counting statistics C208802400031 and Gaussian fits of binned angular data C208802400032 ENDBIB 30 0 C208802400033 COMMON 6 3 C208802400034 EN E-LVL ERR-4 ERR-5 ERR-6 ERR-T C208802400035 MEV MEV PER-CENT PER-CENT PER-CENT PER-CENT C208802400036 21.4 3.368 1.0 4.0 5.0 10.0 C208802400037 ENDCOMMON 3 0 C208802400038 DATA 3 8 C208802400039 ANG-CM DATA ERR-S C208802400040 ADEG NO-DIM NO-DIM C208802400041 37.2 7.92 0.27 C208802400042 40.9 8.64 0.28 C208802400043 44.1 7.24 0.27 C208802400044 47.1 6.09 0.27 C208802400045 50.0 6.03 0.28 C208802400046 52.7 6.92 0.27 C208802400047 55.4 7.48 0.28 C208802400048 57.9 5.45 0.23 C208802400049 ENDDATA 10 0 C208802400050 ENDSUBENT 49 0 C208802499999 ENDENTRY 24 0 C208899999999